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86<br />
The models capture this pattern with the variance of 48% by<br />
the RegCM, 29% by the RSM, and 32% by the WRF. The<br />
spatial patterns are quite consistent with the corresponding<br />
modes from the R2. The spatial correlation coefficients with<br />
the first modes from reanalysis data are 0.8, 0.94, and 0.91<br />
by the RegCM, RSM , and WRF, respectively. The<br />
corresponding temporal correlation coefficients are 0.89,<br />
0.65, and 0.60 by theh RegCM, RSM, and WRF.<br />
system. Part I: Model implementation and sensitivity. Mon.<br />
Wea. Rev, 129, 569–585, 2001.<br />
Dickinson, R., Henderson-Sellers, A. and Kennedy, P.,<br />
Biosphere-atmosphere transfer scheme (bats) version 1e as<br />
coupled to the ncar community climate model, Technical<br />
report, National Center for Atmospheric Research, 1993.<br />
Dudhia, J., Numerical study of convection observed during the<br />
winter monsoon experiment using a mesoscale twodimensional<br />
model. J. Atmos. Sci., 46, 3077-3107, 1989.<br />
Giorgi, F., M. R. Marinucci, and G. T. Bates, Development of a<br />
second-generation regional climate model (RegCM2). Part<br />
Ⅱ : Convective processes and assimilation of lateral<br />
boundary conditions. Mon. Wea. Rev., 121, 2814-2832, 1993.<br />
Grell, G., Prognostic evaluation of assumptions used by cumulus<br />
parameterization, Mon. Wea. Rev, 121, 764-787, 1993.<br />
Holtslag, A.A.M., De Bruijn, E.I.F., Pan, H.-L., A High<br />
Resolution Air Mass Transformation Model for Short-Range<br />
Weather Forecasting. Mon. Wea. Rev. 118, 1561–1575, 1990.<br />
Hong, S.-Y., Y. Noh, and J. Dudhia, A new vertical diffusion<br />
package with an explicit treatment of entrainment processes.<br />
Mon. Wea. Rev., 134, 2318–2341, 2006.<br />
Juang, H.-M. H., S.-Y. Hong, and M. Kanamitsu, The NCEP<br />
regional spectral model: An update, Bull. Amer. Meteor. Soc.,<br />
78, 2125-2143, 1997.<br />
Kain, J., and M. Fritsch, Convective parameterization for<br />
mesoscale models : The Kain- Fritsch scheme. The<br />
representation of cumulus convection in numerical models,<br />
Meteor. Monogr., No. 24, Amer. Meteor. Soc., 165-170,<br />
1993.<br />
Kiehl, J., Hack, J., Bonan, G., Boville, B., Breigleb, B.,<br />
Williamson, D. and Rasch, P., Description of the ncar<br />
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Center for Atmospheric Research,1998.<br />
Figure 2. Same as in Fig. 1 except for precipitation.<br />
Figure 2 compares the EOF patterns and PC time series of<br />
the observed and simulated precipitation. The first<br />
eigenvector of the observed summer precipitation explains<br />
22% of total variance that is smaller than that for<br />
temperature. The interannual variation of precipitation is<br />
more complex and also more difficult to model than<br />
temperature. The first modes of simulated precipitation by<br />
three RCMs explain 21%, 16%, and 18%. The CMAP<br />
precipitation is characterized by positive-negative pattern in<br />
the north-south direction. The RegCM and RSM capture<br />
these patterns, however, the negative area is biased<br />
southward in the RegCM and band-shape is not reproduced<br />
in the RSM compared to the CMAP. The spatial correlations<br />
with the observed mode are 0.43, 0.29, 0.05 for the RegCM,<br />
RSM, and WRF, respectively. The correlation of the PC<br />
time series between the observed and simulated precipitation<br />
for the first mode is about -0.1, 0.33, and 0.23 by the<br />
RegCM, RSM, and WRF, respectively. In contrast to the PC<br />
time series obtained from the surface temperature,<br />
correlation coefficients between the CMAP and simulated<br />
precipitation is low.<br />
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